Chandra Characterization of X-Ray Emission in the Young F-Star Binary System Hd 113766
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CHANDRA CHARACTERIZATION OF X-RAY EMISSION IN THE YOUNG F-STAR BINARY SYSTEM HD 113766 The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation Lisse, C. M. et al. “CHANDRA CHARACTERIZATION OF X-RAY EMISSION IN THE YOUNG F-STAR BINARY SYSTEM HD 113766.” The Astronomical Journal 153.2 (2017): 62. © 2017 The American Astronomical Society As Published http://dx.doi.org/10.3847/1538-3881/153/2/62 Publisher IOP Publishing Version Final published version Citable link http://hdl.handle.net/1721.1/110119 Terms of Use Article is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use. The Astronomical Journal, 153:62 (9pp), 2017 February doi:10.3847/1538-3881/153/2/62 © 2017. The American Astronomical Society. All rights reserved. CHANDRA CHARACTERIZATION OF X-RAY EMISSION IN THE YOUNG F-STAR BINARY SYSTEM HD 113766 C. M. Lisse1, D. J. Christian2, S. J. Wolk3, H. M. Günther4, C. H. Chen5, and C. A. Grady6 1 Planetary Exploration Branch, Space Exploration Sector, Johns Hopkins University Applied Physics Laboratory, 11100 Johns Hopkins Road, Laurel, MD 20723, USA; [email protected] 2 Department of Physics and Astronomy, California State University Northridge, 18111 Nordhoff Street, Northridge, CA 91330, USA; [email protected] 3 Chandra X-ray Center, Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA 02138, USA; [email protected] 4 Massachusetts Institute of Technology, Kavli Institute for Astrophysics and Space Research, 77 Massachusetts Avenue, NE83-569, Cambridge, MA 02139, USA; [email protected] 5 STScI, 3700 San Martin Drive, Baltimore, MD 21218, USA; [email protected] 6 Eureka Scientific and Goddard Space Flight Center, Code 667, NASA-GSFC, Greenbelt, MD 20771, USA; [email protected] Received 2016 January 14; revised 2016 September 8; accepted 2016 September 23; published 2017 January 10 ABSTRACT Using Chandra, we have obtained imaging X-ray spectroscopy of the 10–16 Myr old F-star binary HD 113766. We individually resolve the 1 4 separation binary components for the first time in the X-ray and find a total 0.3–2.0 keV luminosity of 2.2×1029 erg s−1, consistent with previous RASS estimates. We find emission from the easternmost, infrared-bright, dusty member HD 113766A to be only ∼10% that of the western, infrared-faint member HD 113766B. There is no evidence for a 3rd late-type stellar or substellar member of HD 113766 with 25 −1 Lx>6×10 erg s within 2′ of the binary pair. The ratio of the two stars’ X-ray luminosity is consistent with their assignments as F2V and F6V by Pecaut et al. The emission is soft for both stars, kTApec=0.30–0.50 keV, suggesting X-rays produced by stellar rotation and/or convection in young dynamos, but not accretion or outflow shocks, which we rule out. A possible 2.8±0.15 (2σ) hr modulation in the HD 113766B X-ray emission is seen, but at very low confidence and of unknown provenance. Stellar wind drag models corresponding to 29 −1 Lx∼2×10 erg s argue for a 1 mm dust particle lifetime around HD 113766B of only ∼90,0000 years, suggesting that dust around HD 113766B is quickly removed, whereas 1 mm sized dust around HD 113766A can survive for >1.5×106 years. At 1028–1029 erg s−1 X-ray luminosity, astrobiologically important effects, like dust warming and X-ray photolytic organic synthesis, are likely for any circumstellar material in the HD 113766 systems. Key words: astrochemistry – protoplanetary disks – planets and satellites: formation – techniques: spectroscopic – X-rays: stars 1. INTRODUCTION evidence for circumstellar dust orbiting the companion, coeval F-star HD 113766B (Meyer et al. 2001), even though studies of We report here on an analysis of Chandra soft X-ray young stellar clusters (e.g., h and χ Persei, Currie observations of HD 113766, a young (10–16 Myr old, et al. 2007, 2008) would have led us to expect a few similar Mamajek et al. 2002; Chen et al. 2006, 2011; Lisse ) dust-forming collisions every Myr in HD 113766B. et al. 2008; Pecaut et al. 2012 , F-star binary stellar system Late F-stars are typically strong X-ray emitters at a young of near-solar metallicity (Fe/H=−0.1, Nordstrom ) +18/ ( age. In fact, the X-ray luminosity function of the Hyades open et al. 2004 , located at a distance of 123 −14 pc 8.16 mas ( ) ( ) ) ( ) cluster age 600 Myr peaks at late F-stars Stern et al. 1995 . Hipparcos parallax from the Earth Van Leeuwen 2007 . Little While X-ray emission of O to mid B-type stars is attributed to is known about this system in the X-ray, other than it is a dissipating shocks in radiation driven winds, and low-mass reported unresolved RASS source of luminosity 2.1 GKM stars have strong convection leading to an αω or a2 +/− × 29 −1 / 0.7 10 erg s . On the other hand, in the optical IR, dynamo, the origin of emission in late B to early F-stars is the system is very interesting. With two component stars of not so clear. While such stars have a convection zone, the nearly identical age characterized by F spectral types in the ratio of the X-ray to bolometric flux is much smaller than in Sco-Cen star-forming association, attention had been called to typical PMS stars. For example, Collins et al. (2009) find this system, since its association with object IRAS 13037–4545 the 10 Myr debris disk host HD 100453 (A9Ve) to have log ( in the IRAS Point Source Catalog was found Backman & LX/Lbol∼−5.9, whereas the typical value for PMS GKM stars Paresce 1993). More recent work by Meyer et al. (2001), Lisse is about −3.5 (Feigelson et al. 2005). Intermediate mass stars et al. (2008), and Chen et al. (2005, 2006, 2011) have also appear to have softer spectra than their lower-mass confirmed that the system exhibits unobscured photospheres brethren. For example, HD 100453 and the similarly aged 51 and that HD 113766A exhibits one of the largest IR flux Eri (F0V) have coronal temperatures of about 0.2 keV, as excesses measured (LIR/L*=0.015), with no detectable H2 opposed to 1–2 keV for similarly aged GKM stars (Feigelson emission. HD 113766A thus belongs to the class of post-T et al. 2006; Collins et al. 2009). Finally, the “FIP-effect” in Tauri objects characterized by young ages of 5–30 Myr, no which elements with first ionization potential below about leftover primordial gas, and large quantities of excess mid-IR 10 eV are observed to be enhanced in abundance by a factor of emission from circumstellar dust. On the other hand, there is no about 3 in the solar corona (Draker et al. 1995), appears to be 1 The Astronomical Journal, 153:62 (9pp), 2017 February Lisse et al. absent in some F-stars such as τ Boo A (an F7V; Maggio over the l0.5 hr of Chandra observation to within the statistical et al. 2011), and Procyon (an F5IV; Raassen et al. 2002 —but photon noise. There are qualitatively, however, potential see Wood & Laming 2013 for a counter example). variations in the HD 113766B light curve, which could be The twin F-stars in the HD 113766 system are thus an periodic. Analyzing the data for possible sinusoidal variations, interesting and useful couple to study. Close enough (separated we find a number of possible solutions with periods ranging by only 1 4, or 170 AU) to be in the same interstellar medium from 2.61–2.92 hr, with a best-fit solution at 2.87 hr, a peak-to- ( ) 2 ISM environment, far enough separated that they minimally peak amplitude of 20%, and c n = 0.98 for 36 degrees of influence each other’s circumstellar environment inside 100 au, freedom (dof). However, we also find a null periodic solution 2 fi and formed at the same time with about the same total mass, with c n = 1.23, and note that the 95% con dence limit of the 2 they are a natural testbed for trying to understand the c n distribution for 36 dof is 1.42. mechanisms of exosystem formation. As Myr-old F-stars can While it is tempting to assign this periodicity to rotationally be expected to be fast rotators, and more convective and X-ray induced variability, the equatorial velocity implied for a 1.35 −1 active than their main-sequence cousins, we would have RSun F6V star is 423 km s , higher than the predicted breakup naively expected both stars to be rapidly rotating, highly speed for a solar abundance F-star (for M*=1.2–1.6 MSun, −1 convective, and X-ray bright. We thus obtained Chandra vbreakup∼300 km s ). The implied equatorial velocity is also observations of HD 113766 in 2010, because: (a) the system approximately a factor of 2 higher than the fastest known stellar contained a well known and well studied IRAS and WISE debris rotators (Głebocki & Gnaciński 2003; Chen et al. 2011). On the disk, while also being a known RASS source, and therefore other hand, Chen et al. (2011) have listed a value of observable by Chandra, which is a rare combination; (b) using v sin i=93 km s−1 for HD 113766B, and Smith et al.